Missing exponent in "Theoretical Minimum"?

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Discussion Overview

The discussion revolves around a potential typographical error in the Lagrangian presented in "The Theoretical Minimum" related to classical mechanics. Participants examine the application of the Euler-Lagrange equation and question the correctness of the resulting equation, particularly focusing on the presence of exponents in the terms derived from the Lagrangian.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant notes that the Lagrangian includes a term that should have an ##r^2## in the denominator, suggesting a mistake in the differentiation of the potential energy term.
  • Another participant agrees that there should be an ##r^2## in the denominator.
  • A third participant provides clarification on the notation for partial derivatives, indicating that ##\partial## is the correct symbol.
  • A later reply mentions that the original version of the book lacked both exponents in the result, but the online errata has corrected one of them, while the second remains missing.
  • One participant comments on the persistence of typographical errors in published works, emphasizing the importance of verifying formulas independently.

Areas of Agreement / Disagreement

Participants generally agree that there is a typographical error regarding the missing exponent in the denominator, but the discussion also highlights that the issue is not fully resolved as the book contains both incorrect and correct versions of the equation.

Contextual Notes

The discussion reflects uncertainty regarding the accuracy of the published material and the implications of typographical errors on the interpretation of the equations presented.

SamRoss
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TL;DR
Is there a missing exponent in the authors' application of the Euler-Lagrange equation?
In "The Theoretical Minimum" (the one on classical mechanics), on page 218, the authors write a Lagrangian

$$L=\frac m 2 (\dot r^2 +r^2\dot \theta ^2)+\frac {GMm} r$$

They then apply the Euler-Lagrange equation ##\frac d {dt}\frac {dL} {d\dot r}=\frac {dL} {dr}## (I know there should be partial derivatives there but I couldn't find the symbol for it in my Latex primer; if anyone could enlighten me, I'd appreciate it) and wrote the result...

$$\ddot r=r\dot \theta^2-\frac {GM} r$$

My question is, shouldn't the last r in the denominator be squared since it results from differentiating the GMm/r term in the Lagrangian by r?
 
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Indeed, there should be an ##r^2## in the denominator.
 
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...and \partial gives you ##\partial##.
 
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vanhees71 said:
Indeed, there should be an ##r^2## in the denominator.

Thanks, I thought so. The original version of the book apparently lacked both exponents in the result. The online errata for the book shows that, as a correction, the first exponent (above theta dot) was put in but the second exponent is still missing. Weird. However, on the next page of the book the entire equation is written out again, correctly this time. I hadn't moved on to that page before making this post.
 
Well unfortunately typos are very persistent beasts. That's why you havd to carefully check all the formulae yourself in every writing, wherever published!
 
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